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Composite operators and form factors in ${\mathcal N} = 4$ SYM
We construct the most general composite operators of ${\mathcal N} = 4$ SYM in Lorentz harmonic chiral (≈twistor) superspace. The operators are built from the SYM supercurvature which is nonpolynomial in the chiral gauge prepotentials. We reconstruct the full nonchiral dependence of the supercurvatu...
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Lenguaje: | eng |
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2016
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Acceso en línea: | https://dx.doi.org/10.1088/1751-8121/aa72fe http://cds.cern.ch/record/2150957 |
_version_ | 1780950472686829568 |
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author | Chicherin, Dmitry Sokatchev, Emery |
author_facet | Chicherin, Dmitry Sokatchev, Emery |
author_sort | Chicherin, Dmitry |
collection | CERN |
description | We construct the most general composite operators of ${\mathcal N} = 4$ SYM in Lorentz harmonic chiral (≈twistor) superspace. The operators are built from the SYM supercurvature which is nonpolynomial in the chiral gauge prepotentials. We reconstruct the full nonchiral dependence of the supercurvature. We compute all tree-level MHV form factors via the LSZ reduction procedure with on-shell states made of the same supercurvature. |
id | cern-2150957 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2016 |
record_format | invenio |
spelling | cern-21509572021-05-03T20:19:29Zdoi:10.1088/1751-8121/aa72fehttp://cds.cern.ch/record/2150957engChicherin, DmitrySokatchev, EmeryComposite operators and form factors in ${\mathcal N} = 4$ SYMhep-thParticle Physics - TheoryWe construct the most general composite operators of ${\mathcal N} = 4$ SYM in Lorentz harmonic chiral (≈twistor) superspace. The operators are built from the SYM supercurvature which is nonpolynomial in the chiral gauge prepotentials. We reconstruct the full nonchiral dependence of the supercurvature. We compute all tree-level MHV form factors via the LSZ reduction procedure with on-shell states made of the same supercurvature.We construct the most general composite operators of N = 4 SYM in Lorentz harmonic chiral ($\approx$ twistor) superspace. The operators are built from the SYM supercurvature which is nonpolynomial in the chiral gauge prepotentials. We reconstruct the full nonchiral dependence of the supercurvature. We compute all tree-level MHV form factors via the LSZ redcution procedure with on-shell states made of the same supercurvature.CERN-TH-2016-108arXiv:1605.01386oai:cds.cern.ch:21509572016-05-04 |
spellingShingle | hep-th Particle Physics - Theory Chicherin, Dmitry Sokatchev, Emery Composite operators and form factors in ${\mathcal N} = 4$ SYM |
title | Composite operators and form factors in ${\mathcal N} = 4$ SYM |
title_full | Composite operators and form factors in ${\mathcal N} = 4$ SYM |
title_fullStr | Composite operators and form factors in ${\mathcal N} = 4$ SYM |
title_full_unstemmed | Composite operators and form factors in ${\mathcal N} = 4$ SYM |
title_short | Composite operators and form factors in ${\mathcal N} = 4$ SYM |
title_sort | composite operators and form factors in ${\mathcal n} = 4$ sym |
topic | hep-th Particle Physics - Theory |
url | https://dx.doi.org/10.1088/1751-8121/aa72fe http://cds.cern.ch/record/2150957 |
work_keys_str_mv | AT chicherindmitry compositeoperatorsandformfactorsinmathcaln4sym AT sokatchevemery compositeoperatorsandformfactorsinmathcaln4sym |